1959
DOI: 10.1137/1104038
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Waveguides with Random Inhomogeneities and Brownian Motion In the Lobachevsky Plane

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Cited by 100 publications
(102 citation statements)
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“…This observation suggests a heuristic explanation as to why the DMPK equation can still be a good approximation when dL(s) is not distributed as in (16). By using the 'concentration of measure' property on the unitary group, see e.g.…”
Section: Of M(s) Is Haar Distributed In the Unitary Group And Indepenmentioning
confidence: 99%
See 1 more Smart Citation
“…This observation suggests a heuristic explanation as to why the DMPK equation can still be a good approximation when dL(s) is not distributed as in (16). By using the 'concentration of measure' property on the unitary group, see e.g.…”
Section: Of M(s) Is Haar Distributed In the Unitary Group And Indepenmentioning
confidence: 99%
“…The DMPK equation (24) for N = 1 was solved explicitly in [16]. It can be related to Brownian motion in the hyperbolic plane.…”
Section: Hyperbolic Brownian Motionmentioning
confidence: 99%
“…This relationship between reflection eigenvalues and Wigner-Smith delay times is useful because the efTects of absorption have received more attention in the literature than dynamic effects. In particular, the case of a single-mode disordered waveguide with absorption was solved äs early äs 1959, in the course of a radio-engineering problem [17]. The multi-mode case was solved more recently [18,19].…”
Section: Wigner-smith Delay Timementioning
confidence: 99%
“…One such phenomenon that has drawn considerable attention over the years is Anderson localization, originally proposed in the framework of electron transport. Specifically, 50 years ago in the seminal work of Anderson [1,2], it was found that the classical (diffusive) picture was wrong, which assumed that the electrons perform random walks, yielding survival probability decays ∼ 1/ √ t and Ohmic conductance of G ∼ 1/L, where L is the system length (wire length). Due to wave interferences, a total halt of electronic propagation is found instead -leading to a converging non--zero return probability ∼ 1/l ∞ and to an exponential decay of the conductance G ∼ exp(−L/l ∞ ), where l ∞ is the so-called localization length.…”
Section: Introductionmentioning
confidence: 99%